Pickup lens

ABSTRACT

A pickup lens is provided with various aberrations corrected satisfactorily, with a short optical length, and with a sufficient back focus secured. 
     The configuration comprises an aperture diaphragm S 1 , first lens L 1 , second lens L 2 , and third lens L 3 , and is configured by arranging, in order from the object side to the image side, the aperture diaphragm, first lens, second lens, and third lens. The first lens is a lens having positive refractive power, with convex surfaces on the object side and on the image side. The second lens is a lens having negative refractive power, in a meniscus shape with the convex surface on the image side. The third lens is a lens having negative refractive power, in a meniscus shape with the convex surface on the object side. Both of the surfaces of the first lens are aspherical, both of the surfaces of the second lens are aspherical, and both of the surfaces of the third lens are aspherical.

TECHNICAL FIELD

The present invention relates to a pickup lens, and in particular relates to a pickup lens suitable for being mounted in the image input devices of portable telephone sets and personal computers, in digital cameras, CCD cameras for monitoring use, inspection devices, and similar, which use CCDs and CMOS (Complementary Metal Oxide Semiconductor) devices as image pickup elements.

BACKGROUND ART

It is necessary that the above described pickup lens have a short optical length, defined as the distance from the incidence plane on the object side of the pickup lens to the image formation plane (the pickup surface of the CCD or similar). That is, in lens design, measures are necessary to reduce the ratio of the optical length to the combined focal length of the pickup lens. Hereafter, a pickup lens with short optical length and small ratio of optical length to focal length may be called a compact lens.

Taking a portable telephone set as an example, at the least the optical length must be shorter than the thickness of the telephone set main unit. On the other hand, it is convenient that the back focus, defined as the distance from the exit plane on the image side of the pickup lens to the pickup surface, be as long as possible. That is, measures are necessary in the lens design to increase as much as possible the ratio of the back focus to the focal length. This is because of the need to insert a filter, cover glass, and other components between the pickup lens and the pickup surface.

In addition to the above, pickup lenses are of course required to have various aberrations corrected sufficiently that image distortion is not noticed visually, and moreover aberrations should be corrected so as to be sufficiently small as required by the integrated density of the image pickup element (also called “pixels”). That is, the various aberrations must be satisfactorily corrected; hereafter, an image in which aberrations have been satisfactorily corrected may be called a “satisfactory image”.

As described below, pickup lenses with a three-element configuration, suitable for use in image capture equipment employing CCDs, CMOS devices and other solid-state image pickup elements, of which portable computers and videophones are representative, have been disclosed. Such lenses secure a broad angle of view, and can be made compact and lightweight.

Among these, a pickup lens has been disclosed, as a first lens with a three-element configuration, which provides satisfactory images while securing a broad angle of view (see for example Patent Document 1).

However, the shapes of the three lens elements, which are first, second, and third lenses are arranged in order from the object side, are those of a meniscus lens with convex surface on the image side and having positive refractive power as the first lens, a meniscus lens with convex surface facing the object side and having negative refractive power as the second lens, and a convex lens having positive refractive power as the third lens; and the construction has too long an optical length for the back focus length. As a result, the lens cannot be used as a compact lens.

As second through fourth three-element lenses, pickup lenses with a short focal length have been disclosed in which various aberrations have been satisfactorily corrected while securing a broad angle of view (see for example Patent Document 2, Patent Document 3, Patent Document 4).

Similarly to the above-described pickup lens, these pickup lenses also comprise first, second, and third lenses arranged from the object side, with the first lens having positive refractive power, the second lens having negative refractive power, and the third lens having positive refractive power. The combined focal length of the pickup lens is set to be short; but the back focus is long relative to the combined focal length, and the optical length is also too long. In addition, the lenses use a glass material, and so costs are high.

As a fifth three-element lens, a pickup lens has been disclosed which is made compact by employing an aspherical lens and by appropriately setting the power distribution and surface shape (see for example Patent Document 5).

However, in this pickup lens, comprising three lenses which are first, second, and third lenses arranged in order from the object side, the first lens has negative refractive power, the second lens has positive refractive power, and the third lens has negative refractive power; as a result, the pickup lens has a long optical length relative to the combined focal length. In addition, the lenses use a glass material, and so costs are high.

A sixth three-element lens has been disclosed which is a plastic lens with a set of meniscus-shape lenses having concave surfaces directed toward each other, and having at least one plastic lens with an aspherical surface, employing three lenses in the entire lens system to achieve compact size and low cost, and enabling easy suppression of focus movement accompanying temperature changes (see for example Patent Document 6).

However, in this pickup lens, in which first, second, and third lenses are arranged in order from the object side, the first lens has weak refractive power, the second lens has weak refractive power, and the third lens has positive refractive power; consequently the third lens alone is not able to completely compensate for the refractive powers of the first and second lenses, and as a result the back focus is long relative to the combined focal length, and the optical length is also long. However, because the third lens is a glass lens, cost reduction is also inadequate.

A seventh three-element lens has been disclosed in which the lens system is divided into a front group and a rear group, in a telescopic-type lens configuration in which the front group has positive refractive power and the rear group has negative refractive power; the optical length is short, and the lens system is inexpensive (see for example Patent Document 7).

However, in this lens system, in which first, second, and third lenses are arranged in order from the object side, the first lens has negative refractive power, the second lens has positive refractive power, and the third lens has negative refractive power, with a broad gap between the second lens and the third lens. For this reason the optical length is long relative to the combined focal length, and moreover there is the problem that the third lens has large diameter, making the pickup lens unsuitable for use in installation in devices for image input to portable telephone sets and personal computers or in digital cameras, CCD cameras for monitoring, inspection devices, or similar.

An eighth three-element pickup lens, having two positive lenses on the object side as well as a concave negative lens on the image side, both surfaces of which are aspherical, and the negative power of which gradually weakens in moving from the lens center toward the periphery until at the peripheral portion the power is positive, has been disclosed (see for example Patent Document 8).

However, a characteristic of this lens system is that the lens equivalent to the third lens L3 has negative power which gradually weakens in moving from the lens center toward the periphery, such that there exists a position at which the power changes to positive power, at a distance from the lens center in the range from 0.7 times to 1.0 times the effective aperture. In lenses disclosed as embodiments, the positions at which the power changes to positive are at distances from the lens center of 0.96 and 0.97 times the effective apertures, and so set nearly in the peripheral portion of the lens.

If the position at which the power changes to positive is set in the peripheral portion of the lens, then the angle of incidence on the image pickup element of light incident on the vicinity of intersection of the lens optical axis with the pickup surface and on the peripheral portion is nearly perpendicular, while at a position intermediate between the point of intersection of the lens optical axis and the pickup surface and the lens peripheral portion, the angle of incidence on the image pickup element deviates greatly from perpendicular. Hence the angle of incidence of light at positions intermediate from the lens peripheral portion, which are of importance to the image, deviates greatly from the perpendicular, so that light is incident on the image pickup element from an angle oblique to the image pickup element and the amount of reflection at the pickup surface increases, the amount of optical energy reaching the photoelectric conversion face of the image pickup element is reduced, and consequently there is the problem that the image in this portion becomes dark.

As a ninth three-element configuration, a pickup lens has been disclosed in which are arranged, in order from the object side, an aperture diaphragm, a first lens with a biconvex shape having positive refractive power, a second lens with a concave surface directed toward the object side and having negative refractive power, and a third lens with a meniscus shape, with the convex surface directed toward the object side (see for example Patent Document 9).

This lens system is designed such that a satisfactory image can be obtained when the aperture diaphragm is positioned on the object side of the first lens. By positioning the aperture diaphragm on the object side of the first lens, the position of the entrance pupil can be brought close to the object. By this means, there is the characteristic that the principal ray can be made incident on the pickup surface at a nearly perpendicular angle. If the principal ray is made incident on the pickup surface at an oblique angle, shading occurs, in which the amount of light incident on pixels (the image pickup element) positioned in the pickup surface is reduced, and so a problem arises in which the image is darker in the peripheral portions of the picture area.

This problem arises from the fact that when a ray is incident on the image pickup element at an oblique angle to the image pickup element, the amount of light reflected at the surface of the image pickup element increases, and the amount of optical energy reaching the photoelectric conversion face of the image pickup element is reduced. That is, by positioning the aperture diaphragm on the object side of the first lens, a pickup lens design is possible in which shading does not readily occur.

When, in a lens system designed based on such design principles, a diaphragm is further placed between the first lens and the second lens for the purpose of preventing flare, which is a phenomenon in which contrast in the image is decreased, or smear, which is a phenomenon of blurring of the image, the following may occur. Among the principal ray passing through the aperture diaphragm, the principal ray incident at a large angle of incidence to the optical axis of the pickup lens is blocked by this diaphragm. As a result, although stray light which may cause flare or smear and detract from image quality may be blocked, a portion of the principal ray is blocked, as described above, and in some cases the amount of light at the periphery of the image may be decreased, giving rise to the problem of darkness at the peripheral portions of the image.

This lens system has, as the lens equivalent to the third lens, a meniscus lens having positive refractive power; as a characteristic resulting from this, the back focus is relatively short compared with the optical length. Hence, if the back focus is made long in order to insert a filter, cover glass and other components between the pickup lens and the pickup surface, the optical length also becomes long, and there is the problem that the lens system itself becomes too large.

As a tenth three-element lens, a pickup lens has been disclosed in which are arranged, in order from the object side, a first lens with convex shape on the object side and having positive refractive power; a diaphragm; a second lens of a plastic material, at least one surface of which has an aspherical shape, with concave surface on the object side and having positive or negative refractive power; and, a third lens, both surfaces of which have an aspherical shape, with a convex surface on the object side and having positive refractive power (see for example Patent Document 10).

This tenth three-element lens is designed so as to obtain satisfactory images on the assumption that a diaphragm is set between the first and second lenses, and that this diaphragm functions as an aperture diaphragm. Hence when a shutter or similar is placed on the object side of the first lens, the incidence aperture to this lens is narrowed by the shutter or similar. That is, the shutter or similar effectively functions as a diaphragm, so that a portion of the principal ray incident on the diaphragm is blocked. The principal ray incident on the lens at a large angle with the optical axis is a ray which forms the image in the peripheral portion; this ray is blocked by the shutter or similar placed on the object side of the first lens, and so there is the possibility of a problem in which the peripheral portion of the image becomes dark.

In addition, in this lens-system also, similarly to the above-described ninth three-element lens, the lens equivalent to the third lens L3 is a meniscus lens having positive refractive power. Hence in this lens system also, similarly to the ninth three-element lens, if the back focus is made long then the optical length becomes long, and there is the problem that the lens system itself becomes too large.

As an eleventh three-element lens, a pickup lens has been disclosed in which are arranged, in order from the object side, a first lens of a glass material, with a convex surface shape on the object side and having positive refractive power; a second lens with a meniscus shape, formed of a plastic material, at least one surface of which is an aspherical shape, with concave surface on the object side and having positive refractive power; and a third lens, formed from a plastic material, both surfaces of which have an aspherical shape, with convex surface on the object side, and having positive or negative refractive power (see for example Patent Document 11).

The basic configuration of the eleventh three-element lens is the same as that of the tenth three-element lens, and so there are problems similar to those described above for the tenth three-element lens.

As a twelfth three-element lens, a pickup lens has been disclosed in which are placed, in order from the object side, a first lens having at least one surface of which is aspherical in shape, with both surfaces having convex shapes, and having positive refractive power; a diaphragm; a second lens with a meniscus shape, at least one surface of which is aspherical in shape, which has a convex surface on the object side and positive refractive power; and a third lens, both surfaces of which are aspherical in shape, having positive or negative refractive power, formed of a plastic material, and with a convex surface shape on the object side (see for example Patent Document 12).

The basic configuration of the twelfth three-element lens is similar to that of the above-described tenth and eleventh three-lens configuration lenses. Hence there are problems similar to the above-described problems of the tenth and eleventh three-element lenses.

As a thirteenth three-element lens, a pickup lens has been disclosed in which there are, placed in order from the object side, a first lens with a convex surface on the object side and with mainly positive refractive power; a second lens, in a meniscus shape, with convex surface on the image side and having negative refractive power; and a third lens, with a convex surface on the object side, and having positive refractive power. Pickup lenses have been disclosed which have a diaphragm placed on the object side of the first lens, and which have a diaphragm placed between the first lens and the second lens (see for example Patent Document 13).

That is, a pickup lens designed on the assumption that satisfactory images are obtained by causing a diaphragm placed on the object side of the first lens to function as an aperture diaphragm, and a pickup lens designed on the assumption that satisfactory images are obtained by causing a diaphragm placed between the first and second lenses to function as an aperture diaphragm, have been disclosed.

As explained above, when a diaphragm is further placed between the first lens and the second lens in a pickup lens designed so as to obtain satisfactory images on the assumption that a diaphragm placed on the object side of the first lens is made to function as an aperture diaphragm, the principal ray incident at a large incidence angle with the optical axis of the pickup lens among the principal ray passing through the aperture diaphragm is blocked by the additionally placed diaphragm. Similarly, when a diaphragm is placed on the object side of the first lens of a pickup lens designed so as to obtain satisfactory images on the assumption than a diaphragm placed between the first lens and the second lens is made to function as an aperture diaphragm, the principal ray incident at a large incidence angle with the optical axis of the pickup lens among the principal ray passing through the aperture diaphragm is blocked by the additionally placed diaphragm.

As a result, as described above, while stray light which may cause flare, smear or similar, detracting from image quality, can be eliminated, a portion of the principal ray is blocked as described above, and in some cases the amount of light at the periphery of the image may be decreased, giving rise to the problem of darkness at the peripheral portions of the image.

In Patent Document 13, an embodiment is disclosed in which a pickup lens in which an aperture diaphragm is placed on the object side of the first lens, and a pickup lens in which an aperture diaphragm is placed between the first lens and the second lens, are designed mutually independently. That is, the shapes and positions of the first through third lenses are designed so as to obtain a satisfactory image in each case according to the position in which the aperture diaphragm is placed. Hence there is no disclosure of a pickup lens in which a diaphragm is placed on the object side of the first lens, and in addition an aperture diaphragm is placed between the first lens and the second lens. That is, there is no disclosure of a pickup lens in which, in addition to an aperture diaphragm which determines the entrance pupil position, a diaphragm is simultaneously provided for the purpose of preventing flare or smear in order to further improve lens performance.

In the thirteenth three-element lens, similarly to the above-described ninth three-element lens, the lens equivalent to the third lens L3 is a meniscus lens having positive refractive power. Hence in this lens system also, similarly to the ninth three-element lens, if the back focus is made long the optical length will also be long, and so there is the problem that the lens system itself will be too large.

As a fourteenth three-element lens, a pickup lens has been disclosed in which are placed, in order from the object side, a first lens with a convex surface on the object side, having positive refractive power; an aperture diaphragm; a second lens with a meniscus shape, with the convex surface on the image side, having positive refractive index; and a third lens with a concave surface on the image side, having negative refractive power (see for example Patent Document 14).

In this pickup lens, the value of the ratio f₁/f of the focal length f₁ of the first lens to the focal length of the entire pickup lens system is set so as to satisfy 0.8<f₁/f<2.0. Hence the refractive power of the first lens is weak, and the optical length must be made long. Consequently the lens cannot be made compact. Further, a lens having positive refractive power is adopted as the second lens, and the radius of curvature of the surface of this second lens on the image side (the convex surface directed toward the image) must be made small. As a result the lens surface curvature is large, and so die machining becomes difficult.

Patent Document 1: Japanese Unexamined Patent Application Publication No. 2001-075006

Patent Document 2: Japanese Unexamined Patent Application Publication No. 2003-149548

Patent Document 3: Japanese Unexamined Patent Application Publication No. 2002-221659

Patent Document 4: Japanese Unexamined Patent Application Publication No. 2002-244030

Patent Document 5: Japanese Unexamined Patent Application Publication No. 2003-149545

Patent Document 6: Japanese Unexamined Patent Application Publication No. 10-301022

Patent Document 7: Japanese Unexamined Patent Application Publication No. 10-301021

Patent Document 8: Japanese Unexamined Patent Application Publication No. 2003-322792

Patent Document 9: Japanese Unexamined Patent Application Publication No. 2004-4566

Patent Document 10: Japanese Unexamined Patent Application Publication No. 2004-302058

Patent Document 11: Japanese Unexamined Patent Application Publication No. 2004-302059

Patent Document 12: Japanese Unexamined Patent Application Publication No. 2004-302060

Patent Document 13: Japanese Unexamined Patent Application Publication No. 2005-4045

Patent Document 14: Japanese Unexamined Patent Application Publication No. 2005-242286

DISCLOSURE OF THE INVENTION Problems to be Solved by the Invention

Hence an object of the invention is to provide a pickup lens, suitable for mounting in a camera using a CCD or CMOS device as the image capture element, with a short optical length, and back focus as long as possible, and from which satisfactory images can be obtained. A short optical length means, specifically, that the ratio of the optical length to the focal length is small. A long back focus means, specifically, that the ratio of the back focus to the focal length is large.

Further, by realizing all three lenses of a pickup lens of this invention using a plastic material, a pickup lens can be provided at low cost and with light weight. Here, a plastic material is a polymer material which can be formed into a lens through molding by plastic deformation, using heat or pressure or both, and which is transparent to visible light.

Means for Solving the Problems

In order to attain the above-described objects, the pickup lens of a first invention, mounted in an image pickup device comprising a solid-state image pickup element, the length of the diagonal line in the rectangular light-receiving area of which is 2Y, comprises an aperture diaphragm S1, a first lens L1, a second lens L2, and a third lens L3, and is configured by arranging in order, from the object side to the image side, the aperture diaphragm S1, the first lens L1, the second lens L2, and the third lens L3. The first lens L1 is a lens having positive refractive power, with convex surfaces directed toward the object side and toward the image side. The second lens L2 is a lens having negative refractive power, in a meniscus shape with the convex surface directed toward the image side. The third lens L3 is a lens having negative refractive power, with a convex surface directed toward the object side.

Both surfaces of the first lens L1 are aspherical, both surfaces of the second lens L2 are aspherical, and both surfaces of the third lens L3 are aspherical.

Further, this pickup lens satisfies the following conditions (1-1) through (1-4). 0.01<|r ₂ /r ₃|<0.05  (1-1) 0.05<D/f≦0.1  (1-2) 0.6<L/2Y<0.9  (1-3) 0.5<f ₁ /f<0.7  (1-4)

where,

f: combined focal length of the pickup lens

r₂: radius of curvature of the object-side surface of the first lens L1 in the vicinity of the optical axis (radius of curvature at the optical axis)

r₃: radius of curvature of the image-side surface of the first lens L1 in the vicinity of the optical axis (radius of curvature at the optical axis)

D: interval between the second lens L2 and third lens L3 along the optical axis

L: distance in air along the optical axis from the object-side surface of the first lens L1 to the image plane (optical length)

2Y: image height (diagonal-line length of the effective picture area)

f₁: focal length of the first lens L1

The back focus bf, defined as the distance from the exit plane on the image side of the pickup lens to the pickup surface, is here the distance along the optical axis from the image-side surface of the third lens L3 to the image plane. The image height 2Y is the length of the diagonal line in the effective picture area, that is, the length of the diagonal line in the rectangular light-receiving area of the solid-state image pickup element installed at the image plane of the pickup lens.

The pickup lens of a second invention, mounted in an image pickup device comprising a solid-state image pickup element, the length of the diagonal line in the rectangular light-receiving area of which is 2Y, comprises a first lens L1, an aperture diaphragm S2, a second lens L2, and a third lens L3, and is configured by arranging in order, from the object side to the image side, the first lens L1, the aperture diaphragm S2, the second lens L2, and the third lens L3. The first lens L1 is a lens having positive refractive power, with convex surfaces directed toward the object side and toward the image side. The second lens L2 is a lens having negative refractive power, in a meniscus shape with the convex surface directed toward the image side. The third lens L3 is a meniscus lens having negative refractive power, with the convex surface directed toward the object side.

Both surfaces of the first lens L1 are aspherical, both surfaces of the second lens L2 are aspherical, and both surfaces of the third lens L3 are aspherical.

Further, this pickup lens satisfies the following conditions (2-1) through (2-4). 0.01<|r ₁ /r ₂|<0.05  (2-1) 0.05<D/f≦0.1  (2-2) 0.6<L/2Y<0.9  (2-3) 0.5<f ₁ /f<0.7  (2-4)

where,

f: combined focal length of the pickup lens

r₁: radius of curvature of the object-side surface of the first lens L1 in the vicinity of the optical axis (radius of curvature at the optical axis)

r₂: radius of curvature of the image-side surface of the first lens L1 in the vicinity of the optical axis (radius of curvature at the optical axis)

D: interval between the second lens L2 and third lens L3 along the optical axis

L: distance in air along the optical axis from the object-side surface of the first lens L1 to the image plane (optical length)

2Y: image height (diagonal-line length of the effective picture area)

f₁: focal length of the first lens L1

Here, when a filter, cover glass, or other component or other planar sheet is inserted between the third lens L3 and the image plane, the distance in air is calculated to obtain the above-described L taking the portion of this planar sheet as the equivalent distance in air. Similarly in the following explanations, the distance in air refers to the distance calculated taking the equivalent distance in air of the planar sheet portion. That is, if the geometric distance through the planar sheet portion is a, and the refractive index is n, then the distance a is taken to be equivalent to a/n.

The back focus bf, defined as the distance from the exit plane on the image side of the pickup lens to the pickup surface, is here the distance along the optical axis from the image-side surface of the third lens L3 to the image plane. The image height 2Y is the length of the diagonal line of the effective picture area, that is, the length of the diagonal line in the rectangular light-receiving area of the solid-state image pickup element installed at the image plane of the pickup lens.

In the pickup lens of the second invention, an aperture diaphragm S2 is positioned between the first lens L1 and the second lens L2, so that the interval D along the optical axis between the first lens L1 and second lens L2 is defined as follows. The interval D is the sum of the interval from the image-side surface of the first lens L1 to the aperture diaphragm S2 and the interval from the aperture diaphragm S2 to the object-side surface of the second lens L2.

In the pickup lenses of the first and second inventions, it is preferable that the refractive index of the material of the second lens L2 be higher than the refractive indices of the materials of the first lens L1 and third lens L3, and that the Abbe number of the material of the second lens L2 be smaller than the Abbe numbers of the materials of the first lens L1 and third lens L3.

Further, in the pickup lenses of the first and second inventions, it is suitable that the first lens L1, second lens L2, and third lens L3 be formed using materials with Abbe numbers in the range from 30 to 60. Further, the first lens L1 and third lens L3 may be lenses formed using a cycloolefin plastic material, while the second lens L2 may be formed using a fluorene polyester or polycarbonate material.

EFFECTS OF THE INVENTION

By using as the first lens L1 a lens having positive refractive power, with convex surfaces on the object side and on the image side, using as the second lens L2 a lens having negative refractive power, in a meniscus shape with convex surface on the image side, and using as the third lens L3 a lens having negative refractive power, in a meniscus shape with convex surface on the object side, the optical length L can be made short, as explained below.

The advantageous results of pickup lenses of this invention, obtained by satisfying the conditions of equations (1-1) to (1-4) or equations (2-1) to (2-4), are as follows.

The above condition equations (1-1) and (2-1) are condition equations which stipulate the ratio of the radius of curvature at the optical axis of the first surface (the object-side surface) to the radius of curvature at the optical axis of the second surface (the image-side surface) of the first lens L1. If this ratio is larger than the lower limits given by the condition equations (1-1) and (2-1), the back focus bf of the pickup lens is sufficient to enable insertion of cover glass, a filter, or other components between the pickup lens and the pickup surface, and moreover can be set to a length in a range which does not detract from the compactness of the equipment in which the pickup lens is mounted. Moreover, the first surface of the first lens L1 can easily be machined without spherical aberrations becoming too large.

If the ratio of the radius of curvature at the optical axis of the first surface (object-side surface) to the radius of curvature at the optical axis of the second surface (image-side surface) of the first lens L1 is smaller than the upper limit given by the condition equations (1-1) and (2-1), the back focus can be made short, and so a compact pickup lens can be designed. Moreover, the spherical aberration and astigmatic aberration do not take on positive values that are too large. In addition, distortion aberration, although assuming a negative value, does not have too large an absolute value. Consequently these aberrations can be corrected so as to remain within the required ranges by the second lens L2 and third lens L3.

The above condition equations (1-2) and (2-2) are condition equations stipulating the range of values to be taken by the interval D along the optical axis between the first lens L1 and second lens L2, normalized by the combined focal length f of the pickup lens.

If the value of D/f is greater than the lower limits stipulated by the condition equations (1-2) and (2-2), then the incidence angles of rays on the outer periphery which are incident on the image plane are not too large, and so-called “vignetting” in the image plane due to a micro-lens does not occur. Hence the peripheral portions of the image do not become too dark, and a good-quality image is obtained. Further, if the value of D/f is smaller than the upper limit stipulated by the condition equations (1-2) and (2-2), there is no need for a large aperture for the third lens L3, and the overall size of the pickup lens can be kept compact.

The above condition equations (1-3) and (2-3) are condition equations stipulating the range of values to be taken by the ratio of the optical length L to the image height (diagonal-line length in the effective picture area) 2Y.

If the value of L/2Y is greater than the lower limits stipulated by the condition equations (1-3) and (2-3), then the thicknesses of the first lens L1, second lens L2 and third lens L3 can be made equal to or greater than the thicknesses necessary when forming the lenses. That is, when forming the first lens L1, second lens L2 and third lens L3 from resin materials, if the thickness of the lens at the time of injection molding is too thin, then it becomes difficult to inject the resin material so as to flow uniformly into the mold. Hence when forming lenses using a resin material, the lens thickness needs to be at least a certain value. If the ratio L/2Y is larger than the lower limits stipulated by the condition equations (1-3) and (2-3), an adequate lens thickness can be secured.

Further, if the value of L/2Y is smaller than the upper limits stipulated by the condition equations (1-3) and (2-3), then even if the outer diameters of the first lens L1, second lens L2 and third lens L3 are not made so large as to detract from compactness, it is possible to keep the peripheral light quantity ratio of the pickup lens from becoming too small. If the outer diameter can be made small, then the distance in air from the object-side surface to the image-side surface of the first lens L1, that is, the total lens length, can also be made short, through a multiplication effect.

The above condition equations (1-4) and (2-4) are condition equations stipulating the refractive power of the first lens; if the value of f₁/f is smaller than an upper limit, then the refractive power of the first lens L1, which among the first lens L1, second lens L2 and third lens L3 is the only lens having positive refractive power, can be set to an appropriate magnitude; that is, the refractive power of the first lens L1 can be set to a large value, and the overall length of the pickup lens can be made short, within a range in which large aberrations impeding good-quality images do not occur.

If the value of f₁/f is larger than the lower limit, then the positive refractive power of the first lens L1 is not larger than is necessary, and higher-order spherical aberration and coma aberration occurring for the first lens L1 can be made small.

Hence by means of lens configurations for the pickup lenses of the above-described first and second inventions which satisfy the four conditions of the condition equations (1-1) to (1-4) or (2-1) to (2-4), small-size and compact pickup lenses which eliminate the above-described problems, and using which good-quality images are obtained, can be provided.

The pickup lens of the first invention has as a characteristic the positioning of the aperture diaphragm S1, which determines the entrance pupil, in front of the first lens L1, that is, on the object side of the first lens L1. By this means, the entrance pupil can be brought closer to the object side, the principal ray can be made incident on the picture area at an angle close to perpendicular, and the occurrence of shading can be prevented.

The pickup lens of the second invention has as a characteristic the positioning of the aperture diaphragm S2, which determines the entrance pupil, between the first lens L1 and the second lens L2. By this means, the diaphragm S2 functions to eliminate flare occurring at the first lens L1.

In order to modify the F number of the pickup lens, the size of the aperture diaphragm is changed. The pickup lens of the second invention is configured with the aperture diaphragm S2 positioned between the first lens L1 and the second lens L2, and so the F number can be modified merely by replacing the aperture diaphragm S2. However, in order to position an aperture diaphragm in front of the first lens L1, as in the case of the pickup lens of the first invention, it is necessary to return to the stage at which the barrel used to fix the first through third lenses of the pickup lens in place is manufactured, and set the magnitude of the aperture such that the end of the barrel plays the role of the aperture diaphragm S1. That is, each time the F number is changed, the barrel of the pickup lens must be redesigned, and the mold used in manufacturing the barrel of the pickup lens must be remade each time.

As explained above, the pickup lens of the first invention and the pickup lens of the second invention each have different characteristics.

Further, if the refractive index of the material of the second lens L2 is higher than the refractive indices of the materials of the first lens L1 and third lens L3, and if the Abbe number of the material of the second lens L2 is lower than the Abbe numbers of the materials of the first lens L1 and third lens L3, then chromatic/spherical aberration can be effectively reduced.

If the second lens L2 is formed from a fluorene polyester or polycarbonate, and the first lens L1 and third lens L3 are formed using a cycloolefin plastic, then the refractive index of the material of the second lens L2 is higher than the refractive index of the material of the first lens L1 and third lens L3, and the Abbe number of the material of the second lens L2 can be made lower than the Abbe number of the material of the first lens L1 and third lens L3.

The refractive index of cycloolefin plastic is 1.5304, the refractive index of fluorene polyester is 1.607, and the refractive index of polycarbonate is 1.5830, while the Abbe number of cycloolefin plastic is 56.0, the Abbe number of fluorene polyester is 27.0, and the Abbe number of polycarbonate is 30.0, and so these materials can be used in the pickup lenses of this invention.

Cycloolefin plastic, polycarbonate, and fluorene polyester materials are known as materials which are suited to formation of lenses using the injection molding method, which is a well-established manufacturing technology. Of course, the materials are not limited to particular plastic materials, and plastic materials and molded glass materials having Abbe numbers in the range from 30 to 60 can be used.

In the first through eighth Embodiments described below, the first lens L1 and second lens L2 are formed using cycloolefin plastic, and the third lens L3 is formed using fluorene polyester or using polycarbonate.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1 is a cross-sectional view of the pickup lens of the first invention;

FIG. 2 is a cross-sectional view of the pickup lens of a first Embodiment;

FIG. 3 is a diagram of distortion aberration of the pickup lens of the first Embodiment;

FIG. 4 is a diagram of astigmatic aberration of the pickup lens of the first Embodiment;

FIG. 5 is a diagram of the chromatic/spherical aberration of the pickup lens of the first Embodiment;

FIG. 6 is a cross-sectional view of the pickup lens of a second Embodiment;

FIG. 7 is a diagram of distortion aberration of the pickup lens of the second Embodiment;

FIG. 8 is a diagram of astigmatic aberration of the pickup lens of the second Embodiment;

FIG. 9 is a diagram of the chromatic/spherical aberration of the pickup lens of the second Embodiment;

FIG. 10 is a cross-sectional view of the pickup lens of a third Embodiment;

FIG. 11 is a diagram of distortion aberration of the pickup lens of the third Embodiment;

FIG. 12 is a diagram of astigmatic aberration of the pickup lens of the third Embodiment;

FIG. 13 is a diagram of the chromatic/spherical aberration of the pickup lens of the third Embodiment;

FIG. 14 is a cross-sectional view of the pickup lens of a fourth Embodiment;

FIG. 15 is a diagram of distortion aberration of the pickup lens of the fourth Embodiment;

FIG. 16 is a diagram of astigmatic aberration of the pickup lens of the fourth Embodiment;

FIG. 17 is a diagram of the chromatic/spherical aberration of the pickup lens of the fourth Embodiment;

FIG. 18 is a cross-sectional view of the pickup lens of the second invention;

FIG. 19 is a cross-sectional view of the pickup lens of a fifth Embodiment;

FIG. 20 is a diagram of distortion aberration of the pickup lens of the fifth Embodiment;

FIG. 21 is a diagram of astigmatic aberration of the pickup lens of the fifth Embodiment;

FIG. 22 is a diagram of the chromatic/spherical aberration of the pickup lens of the fifth Embodiment;

FIG. 23 is a cross-sectional view of the pickup lens of a sixth Embodiment;

FIG. 24 is a diagram of distortion aberration of the pickup lens of the sixth Embodiment;

FIG. 25 is a diagram of astigmatic aberration of the pickup lens of the sixth Embodiment;

FIG. 26 is a diagram of the chromatic/spherical aberration of the pickup lens of the sixth Embodiment;

FIG. 27 is a cross-sectional view of the pickup lens of a seventh Embodiment;

FIG. 28 is a diagram of distortion aberration of the pickup lens of the seventh Embodiment;

FIG. 29 is a diagram of astigmatic aberration of the pickup lens of the seventh Embodiment;

FIG. 30 is a diagram of the chromatic/spherical aberration of the pickup lens of the seventh Embodiment;

FIG. 31 is a cross-sectional view of the pickup lens of an eighth Embodiment;

FIG. 32 is a diagram of distortion aberration of the pickup lens of the eighth Embodiment;

FIG. 33 is a diagram of astigmatic aberration of the pickup lens of the eighth Embodiment; and,

FIG. 34 is a diagram of the chromatic/spherical aberration of the pickup lens of the eighth Embodiment.

EXPLANATIONS OF LETTERS OR NUMERALS

-   10 imaging element -   S1, S2 diaphragms -   L1 first lens -   L2 second lens -   L3 third lens -   r_(i) optical axial radius of curvature of i^(th) surface -   d_(i) distance from intersection between i^(th) surface and optical

BEST MODE FOR CARRYING OUT THE INVENTION

Below, aspects of the invention are explained, referring to the drawings. These drawings merely show in summary manner the shapes, sizes and positional relations of constituent components to an extent enabling understanding of the invention; moreover, the numerical conditions and other conditions explained below are merely suitable examples, and this invention is in no way limited to these aspects.

FIG. 1 and FIG. 18 show the configurations of the pickup lenses of the first and second inventions respectively. The surface numbers, intervals between surfaces, and other symbols defined in FIG. 1 and FIG. 18 are used in common in FIG. 2, FIG. 6, FIG. 10, FIG. 14, FIG. 19, FIG. 23, FIG. 27, and FIG. 31.

Counting from the object side, the first, second, and third lenses are represented by L1, L2, and L3, respectively, and aperture diaphragms are represented by S1 and S2. The aperture diaphragm placed in front of the first lens L1 is indicated by S1, and the aperture diaphragm placed between the first lens L1 and the second lens L2 is indicated by S2.

In addition to using variables r_(i) (i=1, 2, 3, . . . , 8) as indicating the radius of curvature at the optical axis, so long as there is no chance for misunderstanding, similar symbols are also used to distinguish lenses, cover glass, and the pickup surface (for example, with r₁ used to represent the object-side surface of the first lens).

The r_(i) (i=1, 2, 3, . . . , 8) and d_(i) (i=1, 2, 3, . . . , 7) and other parameters used in the figures are provided with specific numerical values in Table 1 through Table 8 below. Values of the subscript i are assigned in order moving from the object side to the image side, corresponding to the lens surface number, or to the lens thickness or interval between lenses, and similar.

That is, r_(i) is the radius of curvature at the optical axis of the ith surface; d_(i) is the distance from the ith surface to the i+1th surface; N_(i) is the refractive index of the material of the lens comprising the ith surface and i+1th surface; and ν_(i) is the Abbe number of the material of the lens from the ith surface to the i+1th surface.

In FIG. 1 and FIG. 18, line segments indicate the aperture portions of diaphragms. This is in order to clearly show the point of intersection of the diaphragm plane with the optical axis, in order to define the distance from a lens surface to the diaphragm plane. Further, in FIG. 2, FIG. 6, FIG. 10, FIG. 14, FIG. 19, FIG. 23, FIG. 27 and FIG. 31, which are cross-sectional views of the pickup lenses of the first through eighth Embodiments, respectively, in contrast with the above FIG. 1 and FIG. 18, the diaphragm aperture portion is opened, and two straight lines which start at the edges of the aperture portion are used to indicate the body of the diaphragm which blocks light. This is because of the need to open the aperture portion of the diaphragm, indicating the state of the diaphragm, in order to draw the principal ray and other rays.

The optical length L is, in a pickup lens of the first invention, the distance from the diaphragm S1 to the pickup surface, and in a pickup lens of the second invention, the distance from the point at which the object-side surface of the first lens and the optical axis intersect to the pickup surface. The back focus bf is the distance along the optical axis from the image-side surface of the third lens L3 to the pickup surface.

Aspherical surface data is indicated in the respective surface number columns in Table 1 through Table 8. The planes of the diaphragms S1 and S2 and the pickup surface are planes, and so the radius of curvature is given as infinity, ∞.

The aspherical surfaces used in this invention are described by the following equation. Z=ch ²/[1+[1−(1+k)c ² h ²]^(+1/2) ]+A ₀ h ⁴ +B ₀ h ⁶ +C ₀ h ⁸ +D ₀ h ¹⁰

where Z is the depth from the plane tangent at the surface vertex, c is the curvature of the surface in the vicinity of the optical axis, h is the distance from the optical axis, k is the conic constant, A₀ is the fourth-order aspheric coefficient, B₀ is the sixth-order aspheric coefficient, C₀ is the eighth-order aspheric coefficient, and D₀ is the tenth-order aspheric coefficient.

In Table 1 through Table 8 in this Specification, numerical values of aspheric coefficients employ an exponent notation in which, for example, “e-1” signifies “10 to the −1 power”. Also, values given as focal lengths f are combined focal lengths of the lens system comprising the first through third lenses.

Below, the first through fourth Embodiments are explained referring to FIG. 1 through FIG. 17, and fifth through eighth Embodiments are explained referring to FIG. 18 through FIG. 34.

The distortion aberration curves shown in FIG. 3, FIG. 7, FIG. 11, FIG. 15, FIG. 20, FIG. 24, FIG. 28, and FIG. 32 show the aberration amount (the amount by which the tangent condition is not satisfied, expressed as a percentage along the horizontal axis) versus the distance from the optical axis (expressed as a percentage along the vertical axis, with the maximum distance from the optical axis within the image plane equal to 100). The astigmatic aberration curves shown in FIG. 4, FIG. 8, FIG. 12, FIG. 16, FIG. 21, FIG. 25, FIG. 29, and FIG. 33 show the amounts of aberration along the horizontal axis (in mm units) for a distance from the optical axis, similarly to a distortion aberration curve. Astigmatism is represented as aberration amounts (in mm units) in the meridional plane and in the sagittal plane. The chromatic/spherical aberration curves shown in FIG. 5, FIG. 9, FIG. 13, FIG. 17, FIG. 22, FIG. 26, FIG. 30, and FIG. 34 show the amount of aberration along the horizontal axis (in mm units) for a distance of incidence h (F number) along the vertical axis.

In a chromatic/spherical aberration curve, aberration amounts are shown for the C line (light of wavelength 656.3 nm), the d line (light of wavelength 587.6 nm), the e line (light of wavelength 546.1 nm), the F line (light of wavelength 486.1 nm), and the g line (light of wavelength 435.8 nm). The refractive index is the refractive index for the d line (light of wavelength 587.6 nm).

Below, the radii of curvature of component lenses (mm units), intervals between lens surfaces (mm units), refractive indices of lens materials, Abbe numbers of lens materials, focal lengths, F numbers, and aspheric coefficients are listed for the first through eighth Embodiments in Table 1 through Table 8. In the first through eighth Embodiments, the focal lengths of the first lens L1, second lens L2 and third lens L3 are indicated by f₁, f₂ and f₃ respectively. In all cases in the first through eighth Embodiments, f₁ is positive, and f₂ and f₃ are negative. That is, the first lens L1 is a lens having positive refractive power, and the second lens L2 and third lens L3 are lenses having negative refractive power. The values of the combined focal length f of the pickup lenses are normalized to 1.00 mm.

The radii of curvature at the optical axis r_(i) (i=1, 2, 3, . . . , 8) are positive values when the shape is convex on the object side, and negative values when the shape is convex on the image side. From the signs of the values of the radii of curvature of the surfaces comprising the lenses, it is possible to ascertain that the first lens L1 is a convex lens having convex surfaces on the object side and on the image side, that the second lens L2 is a meniscus lens having a convex surface on the image side, and that the third lens L3 is a convex lens having convex surfaces on the object side and on the image side.

Below, characteristics of each of the embodiments are described. In the first through eighth Embodiments, ZEONEX E48R (ZEONEX is a registered trademark, and E48R is a product number, of Nippon Zeon Co., Ltd.), which is a cycloolefin plastic, was employed in the first lens L1 and third lens L3. Fluorene polyester or polycarbonate was used as the material of the second lens L2.

The refractive index of ZEONEX E48R for the d line is 1.5304, and the refractive indices of fluorine polyester and of polycarbonate for the d line are respectively 1.607 and 1.5830. Further, the Abbe number of ZEONEX is 56.0, and the Abbe numbers of fluorine polyester and of polycarbonate are respectively 27.0 and 30.0.

Both surfaces of the first lens L1, second lens L2, and third lens L3 are aspherical.

First Invention

As shown in FIG. 1, the pickup lens of the first invention comprises an aperture diaphragm S1, first lens L1, second lens L2, and third lens L3, and is configured by arranging, in order from the object side toward the image side, the aperture diaphragm S1, first lens L1, second lens L2, and third lens L3. The radii of curvature (mm units), intervals between lens surfaces (mm units), refractive indices of lens materials, Abbe numbers of lens materials, focal lengths, F numbers, aspheric coefficients and similar of the component lenses comprised by the first through fourth Embodiments of the pickup lens of the first invention, are listed in Table 1 through Table 4 respectively. The quantity D representing the interval along the optical axis between the second lens L2 and the third lens L3 corresponds to d₅ in Table 1 through Table 4.

TABLE 1 First Embodiment Radius of Refractive Abbe Aspheric Coefficients Curvature(r_(i)) Interval(d_(i)) Index(N_(i)) Number(ν_(i)) K A_(o) B_(o) C_(o) D_(o) r₁ = ∞ d₁ = 0.0000 r₂ = 0.356 1.667 −6.182 −4.554e+1  −1.638e+3 −9.416e+4 d₂ = 0.1827 N₂ = 1.5304 ν₂ = 56.0 r₃ = −17.782  2.624e+3 −7.506 1.246e+1 −6.110e+3 −4.034e+4 d₃ = 0.1167 r₄ = −0.219  7.041e−2 1.077e+1 5.294e+2 −4.468e+3 −1.464e+5 d₄ = 0.1251 N₄ = 1.6070 ν₄ = 27.0 r₅ = −0.344 −6.306e−1 4.833e−2 4.434e+2 −3.444e+3  3.611e+3 d₅ = 0.1000 r₆ = 0.631 −3.669e+1 −4.933 5.289e+1 −2.673e+2  4.585e+2 d₆ = 0.2074 N₆ = 1.5304 ν₆ = 56.0 r₇ = 0.537 −1.751e+1 −4.574 2.023e+1 −5.507e+1  1.005e+1 d₇ = 0.3889 r₈ = ∞ Focal Length f = 1.00 mm F Number F_(no) = 3.4 Image Height 2Y = 1.28 mm f₁ = 0.66 mm f₂ = −1.58 mm f₃ = 28.53 mm

TABLE 2 Second Embodiment Radius of Refractive Abbe Aspheric Coefficients Curvature(r_(i)) Interval(d_(i)) Index(N_(i)) Number(ν_(i)) K A_(o) B_(o) C_(o) D_(o) r₁ = ∞ d₁ = 0.0000 r₂ = 0.356 1.657 −6.318 −4.259e+1  −1.573e+3 −1.003e+5 d₂ = 0.1827 N₂ = 1.5304 ν₂ = 56.0 r₃ = −17.782  1.039e+4 −7.887 1.308e+1 −5.938e+3 −5.026e+4 d₃ = 0.1167 r₄ = −0.217  9.362e−2 1.061e+1 5.293e+2 −4.194e+3 −1.679e+5 d₄ = 0.1260 N₄ = 1.5830 ν₄ = 30.0 r₅ = −0.347 −6.665e−1 2.110e−1 4.439e+2 −3.472e+3  2.977e+3 d₅ = 0.1000 r₆ = 0.622 −3.304e+1 −4.719 5.254e+1 −2.687e+2  4.934e+2 d₆ = 0.2074 N₆ = 1.5304 ν₆ = 56.0 r₇ = 0.537 −1.674e+1 −4.460 1.976e+1 −5.375e+1  1.997e+1 d₇ = 0.3861 r₈ = ∞ Focal Length f = 1.00 mm F Number F_(no) = 3.4 Image Height 2Y = 1.28 mm f₁ = 0.66 mm f₂ = −1.53 mm f₃ = −46.94 mm

TABLE 3 Third Embodiment Radius of Refractive Abbe Aspheric Coefficients Curvature(r_(i)) Interval(d_(i)) Index(N_(i)) Number(ν_(i)) K A_(o) B_(o) C_(o) D_(o) r₁ = ∞ d₁ = 0.0000 r₂ = 0.356  1.299 −5.360 −6.871e+1   1.240e+3 −1.044e+5 d₂ = 0.1826 N₂ = 1.5300 ν₂ = 56.0 r₃ = −8.887  4.898e+2 −6.933 7.254e+1 −5.561e+3 −8.331e+3 d₃ = 0.1167 r₄ = −0.227 −1.267e−1 1.717e+1 4.396e+2 −7.141e+3 −7.639e+4 d₄ = 0.1244 N₄ = 1.5830 ν₄ = 30.0 r₅ = −0.318 −2.311  2.888 4.437e+2 −2.915e+3 −9.266e+3 d₅ = 0.0800 r₆ = 1.092 −1.866e+2 −5.342 6.070e+1 −2.726e+2  4.963e+2 d₆ = 0.2073 N₆ = 1.5300 ν₆ = 56.0 r₇ = 0.568 −2.238e+1 −5.370 2.847e+1 −1.228e+2  1.880e+2 d₇ = 0.3810 r₈ = ∞ Focal Length f = 1.00 mm F Number F_(no) = 3.4 Image Height 2Y = 1.28 mm f₁ = 0.65 mm f₂ = −2.71 mm f₃ = −2.59 mm

TABLE 4 Fourth Embodiment Radius of Refractive Abbe Aspheric Coefficients Curvature(r_(i)) Interval(d_(i)) Index(N_(i)) Number(ν_(i)) K A_(o) B_(o) C_(o) D_(o) r₁ = ∞ d₁ = 0.0000 r₂ = 0.356  1.300 −5.677 −6.000e+1   3.486e+2 −1.118e+5 d₂ = 0.1826 N₂ = 1.5300 ν₂ = 56.0 r₃ = −8.887  2.300e+3 −8.034 3.438e+1 −5.859e+3 −3.092e+4 d₃ = 0.1167 r₄ = −0.216 −1.037e−1 1.815e+1 4.097e+2 −5.808e+3 −1.507e+5 d₄ = 0.1244 N₄ = 1.5830 ν₄ = 30.0 r₅ = −0.303 −2.117  3.302 4.494e+2 −3.010e+3 −1.106e+4 d₅ = 0.0511 r₆ = 1.186 −1.850e+2 −5.012 6.129e+1 −2.753e+2  4.580e+2 d₆ = 0.2073 N₆ = 1.5300 ν₆ = 56.0 r₇ = 0.665 −2.815e+1 −5.570 2.695e+1 −1.195e+2  1.852e+2 d₇ = 0.4222 r₈ = ∞ Focal Length f = 1.00 mm F Number F_(no) = 3.4 Image Height 2Y = 1.28 mm f₁ = 0.65 mm f₂ = −2.67 mm f₃ = −3.32 mm

FIRST EMBODIMENT

Zeonex E48R was used as the material of the first lens L1 and third lens L3, while fluorene polyester EP-4000 (EP-4000 is a product number of Mitsubishi Gas Chemical Co., Inc.) was used as the material of the second lens L2.

(A) The object-side radius of curvature r₂ of the first lens L1 is r₂=0.356 mm.

(B) The image-side radius of curvature r₃ of the first lens L1 is r₃=−17.782 mm.

(C) The interval D along the optical axis between the second lens L2 and the third lens L3 is D (=d₅)=0.1000 mm.

(D) The optical length L is L=1.121 mm.

(E) The image height (length of the diagonal line in the rectangular light-receiving area) 2Y is 2Y=2×0.64=1.28 mm.

(F) The focal length f₁ of the first lens L1 is f₁=0.66 mm.

Hence: |r ₂ /r ₃|=10.356/−17.782|=0.020,  (1-1) D/f=0.1000/1.00=0.1000,  (1-2) L/2Y=1.121/1.28=0.876, and  (1-3) f ₁ /f=0.66/1.00=0.66.  (1-4)

Hence the lens system of the first Embodiment satisfies each of the following condition equations (1-1) to (1-4). 0.01<|r ₂ /r ₃|1<0.05  (1-1) 0.05<D/f≦0.1  (1-2) 0.6<L/2Y<0.9  (1-3) 0.5<f ₁ /f<0.7  (1-4)

In the following, the condition equations of the first invention are taken to refer to the above four equations (1-1) through (1-4).

As shown in Table 1, the diaphragm S1 is provided at the position of the point of intersection of the first surface (object-side surface) of the first lens L1 with the optical axis. That is, because the diaphragm surface is planar, in Table 1 r₁=∞, and so the diaphragm S1 is placed at the position of the plane r₁. The F number is 3.4.

FIG. 2 is a cross-sectional view of the pickup lens of the first Embodiment. A sufficiently long back focus relative to the 1.00 mm focal length of 0.389 mm is secured.

FIG. 3 shows the distortion aberration curve 20, FIG. 4 shows the astigmatic aberration curves (the aberration curve 22 in the meridional plane and the aberration curve 24 in the sagittal plane), and FIG. 5 shows the chromatic/spherical aberration curves (the aberration curve 26 for the C line, aberration curve 28 for the d line, aberration curve 30 for the e line, aberration curve 32 for the F line, and aberration curve 34 for the g line).

The vertical axes of the aberration curves in FIG. 3 and FIG. 4 indicate the distance from the optical axis of the image height, as a percentage. In FIG. 3 and FIG. 4, 100% on the vertical axes corresponds to 0.640 mm. The vertical axis for the aberration curve in FIG. 5 indicates the distance of incidence h (F number); the maximum corresponds to 3.4. The horizontal axis in FIG. 5 indicates the aberration magnitude.

The absolute value of distortion aberration is maximum, at 0.2640%, at an image height of 60% (image height 0.384 mm). At image heights of 0.640 mm or less, the absolute value of the aberration is within 0.2640%.

The absolute value of astigmatic aberration is maximum in the meridional plane, at 0.0513 mm, at an image height of 100% (image height 0.640 mm). At image heights of 0.640 mm or less, the absolute value of the aberration is within 0.0513 mm.

The absolute value of chromatic/spherical aberration is maximum, at 0.0114 mm, for the g line of the aberration curve 34 at a distance of incidence h of 30%, and the absolute value of the aberration is within 0.0114 mm.

SECOND EMBODIMENT

ZEONEX E48R was used as the material of the first lens L1 and third lens L3, and polycarbonate was used as the material of the second lens L2.

(A) The object-side radius of curvature r₂ of the first lens L1 is r₂=0.356 mm.

(B) The image-side radius of curvature r₃ of the first lens L1 is r₃=−17.782 mm.

(C) The interval D along the optical axis between the second lens L2 and the third lens L3 is D (=d₅)=0.1000 mm.

(D) The optical length L is L=1.119 mm.

(E) The image height (length of the diagonal line in the rectangular light-receiving area) 2Y is 2Y=2×0.64=1.28 mm.

(F) The focal length f₁ of the first lens L1 is f₁=0.66 mm.

Hence: |r ₂ /r ₃|=|0.3561/−17.782|=0.020,  (1-1) D/f=0.1000/1.00=0.1000,  (1-2) L/2Y=1.119/1.28=0.874, and  (1-3) f ₁ /f=0.66/1.00=0.66.  (1-4)

Hence the lens system of the second Embodiment satisfies each of the following condition equations (1-1) through (1-4). 0.01<|r ₂ /r ₃|<0.05  (1-1) 0.05<D/f≦0.1  (1-2) 0.6<L/2Y<0.9  (1-3) 0.5<f ₁ /f<0.7  (1-4)

In the following, the condition equations of the first invention are taken to refer to the above four equations (1-1) through (1-4).

As shown in Table 2, the diaphragm S1 is provided at the position of the point of intersection of the first surface (object-side surface) of the first lens L1 with the optical axis. That is, the diaphragm surface is planar, and so in Table 2 r₁=∞, and the diaphragm S1 is positioned at the position of the plane r₁. The F number is 3.4.

FIG. 6 is a cross-sectional view of the pickup lens of the second Embodiment. A sufficiently long back focus relative to the 1.00 mm focal length of 0.386 mm is secured.

FIG. 7 shows the distortion aberration curve 36, FIG. 8 shows the astigmatic aberration curves (the aberration curve 38 in the meridional plane and the aberration curve 40 in the sagittal plane), and FIG. 9 shows the chromatic/spherical aberration curves (the aberration curve 42 for the C line, aberration curve 44 for the d line, aberration curve 46 for the e line, aberration curve 48 for the F line, and aberration curve 50 for the g line).

The vertical axes of the aberration curves in FIG. 7 and FIG. 8 indicate the distance from the optical axis of the image height, as a percentage. In FIG. 7 and FIG. 8, 100% on the vertical axes corresponds to 0.640 mm. The vertical axis for the aberration curve in FIG. 9 indicates the distance of incidence h (F number); the maximum corresponds to 3.4. The horizontal axis in FIG. 9 indicates the aberration magnitude.

The absolute value of distortion aberration is maximum, at 0.2203%, at an image height of 60% (image height 0.384 mm). At image heights of 0.640 mm or less, the absolute value of the aberration is within 0.2203%.

The absolute value of astigmatic aberration is maximum in the meridional plane, at 0.0234 mm, at an image height of 100% (image height 0.640 mm). At image heights of 0.640 mm or less, the absolute value of the aberration is within 0.0234 mm.

The absolute value of chromatic/spherical aberration is maximum, at 0.0129 mm, for the g line of the aberration curve 50 at a distance of incidence h of 30%, and the absolute value of the aberration is within 0.0129 mm.

THIRD EMBODIMENT

ZEONEX E48R was used as the material of the first lens L1 and third lens L3, and polycarbonate was used as the material of the second lens L2.

(A) The object-side radius of curvature r₂ of the first lens L1 is r₂=0.356 mm.

(B) The image-side radius of curvature r₃ of the first lens L1 is r₃=−8.887 mm.

(C) The interval D along the optical axis between the second lens L2 and the third lens L3 is D (=d₅)=0.08 mm.

(D) The optical length L is L=1.092 mm.

(E) The image height (length of the diagonal line in the rectangular light-receiving area) 2Y is 2Y=2×0.64=1.28 mm.

(F) The focal length f₁ of the first lens L1 is f₁=0.65 mm.

Hence: |r ₂ /r ₃|=|0.356/−8.887|=0.04,  (1-1) D/f=0.1000/1.00=0.08,  (1-2) L/2Y=1.092/1.28=0.8531, and  (1-3) f ₁ /f=0.65/1.00=0.65.  (1-4)

Hence the lens system of the third Embodiment satisfies each of the following condition equations (1-1) through (1-4). 0.01<|r ₂ /r ₃|<0.05  (1-1) 0.05<D/f≦0.1  (1-2) 0.6<L/2Y<0.9  (1-3) 0.5<f ₁ /f<0.7  (1-4)

In the following, the condition equations of the first invention are taken to refer to the above four equations (1-1) through (1-4).

As shown in Table 3, the diaphragm S1 is provided at the position of the point of intersection of the first surface (object-side surface) of the first lens L1 with the optical axis. That is, the diaphragm surface is planar, and so in Table 3 r₁=∞, and the diaphragm S1 is positioned at the position of the plane r₁. The F number is 3.4.

FIG. 10 is a cross-sectional view of the pickup lens of the third Embodiment. A sufficiently long back focus relative to the 1.00 mm focal length of 0.381 mm is secured.

FIG. 11 shows the distortion aberration curve 52, FIG. 12 shows the astigmatic aberration curves (the aberration curve 54 in the meridional plane and the aberration curve 56 in the sagittal plane), and FIG. 13 shows the chromatic/spherical aberration curves (the aberration curve 58 for the C line, aberration curve 60 for the d line, aberration curve 62 for the e line, aberration curve 64 for the F line, and aberration curve 66 for the g line).

The vertical axes of the aberration curves in FIG. 11 and FIG. 12 indicate the distance from the optical axis of the image height, as a percentage. In FIG. 11 and FIG. 12, 100% on the vertical axes corresponds to 0.640 mm. The vertical axis for the aberration curve in FIG. 13 indicates the distance of incidence h (F number); the maximum corresponds to 3.4. The horizontal axis in FIG. 13 indicates the aberration magnitude.

The absolute value of distortion aberration is maximum, at 0.5710%, at an image height of 100% (image height 0.640 mm). At image heights of 0.640 mm or less, the absolute value of the aberration is within 0.5710%.

The absolute value of astigmatic aberration is maximum in the meridional plane, at 0.0115 mm, at an image height of 100% (image height 0.640 mm). At image heights of 0.640 mm or less, the absolute value of the aberration is within 0.0115 mm.

The absolute value of chromatic/spherical aberration is maximum, at 0.0154 mm, for the g line of the aberration curve 66 at a distance of incidence h of 30%, and the absolute value of the aberration is within 0.0154 mm.

FOURTH EMBODIMENT

ZEONEX E48R was used as the material of the first lens L1 and third lens L3, and polycarbonate was used as the material of the second lens L2.

(A) The object-side radius of curvature r₂ of the first lens L1 is r₂=0.356 mm.

(B) The image-side radius of curvature r₃ of the first lens L1 is r₃=−8.887 mm.

(C) The interval D along the optical axis between the second lens L2 and the third lens L3 is D (=d₅)=0.0511 mm.

(D) The optical length L is L=1.1043 mm.

(E) The image height (length of the diagonal line in the rectangular light-receiving area) 2Y is 2Y=2×0.64=1.28 mm.

(F) The focal length f₁ of the first lens L1 is f₁=0.65 mm.

Hence: |r ₂ /r ₃|=|0.356/−8.887|=0.04,  (1-1) D/f=0.0511/1.00=0.0511,  (1-2) L/2Y=1.104/1.28=0.8627, and  (1-3) f ₁ /f=0.65/1.00=0.65.  (1-4)

Hence the lens system of the fourth Embodiment satisfies each of the following condition equations (1-1) through (1-4). 0.01<|r ₂ /r ₃|<0.05  (1-1) 0.05<D/f≦0.1  (1-2) 0.6<L/2Y<0.9  (1-3) 0.5<f ₁ /f<0.7  (1-4)

In the following, the condition equations of the first invention are taken to refer to the above four equations (1-1) through (1-4).

As shown in Table 4, the diaphragm S1 is provided at the position of the point of intersection of the first surface (object-side surface) of the first lens L1 with the optical axis. That is, the diaphragm surface is planar, and so in Table 4 r₁=∞, and the diaphragm S1 is positioned at the position of the plane r₁. The F number is 3.4.

FIG. 14 is a cross-sectional view of the pickup lens of the fourth Embodiment. A sufficiently long back focus relative to the 1.00 mm focal length of 0.422 mm is secured.

FIG. 15 shows the distortion aberration curve 68, FIG. 16 shows the astigmatic aberration curves (the aberration curve 70 in the meridional plane and the aberration curve 72 in the sagittal plane), and FIG. 17 shows the chromatic/spherical aberration curves (the aberration curve 74 for the C line, aberration Curve 76 for the d line, aberration curve 78 for the e line, aberration curve 80 for the F line, and aberration curve 82 for the g line).

The vertical axes of the aberration curves in FIG. 15 and FIG. 16 indicate the distance from the optical axis of the image height, as a percentage. In FIG. 15 and FIG. 16, 100% on the vertical axes corresponds to 0.639 mm. The vertical axis for the aberration curve in FIG. 17 indicates the distance of incidence h (F number); the maximum corresponds to 3.4. The horizontal axis in FIG. 17 indicates the aberration magnitude.

The absolute value of distortion aberration is maximum, at 0.5428%, at an image height of 100% (image height 0.639 mm). At image heights of 0.639 mm or less, the absolute value of the aberration is within 0.5428%.

The absolute value of astigmatic aberration is maximum in the meridional plane, at 0.0152 mm, at an image height of 80% (image height 0.512 mm). At image heights of 0.639 mm or less, the absolute value of the aberration is within 0.0152 mm.

The absolute value of chromatic/spherical aberration is maximum, at 0.0153 mm, for the g line of the aberration curve 82 at a distance of incidence h of 30%, and the absolute value of the aberration is within 0.0153 mm.

Second Invention

As shown in FIG. 18, the pickup lens of the second invention comprises a first lens L1, aperture diaphragm S2, second lens L2, and third lens L3, and is configured by arranging, in order from the object side toward the image side, the first lens L1, aperture diaphragm S2, second lens L2, and third lens L3. The radii of curvature (mm units), intervals between lens surfaces (mm units), refractive indices of lens materials, Abbe numbers of lens materials, focal lengths, F numbers, aspheric coefficients and similar of the component lenses comprised by the fifth through eighth Embodiments of the pickup lens of the second invention, are listed in Table 5 through Table 8 respectively. The quantity D representing the interval along the optical axis between the second lens L2 and the third lens L3 corresponds to d₅ in Table 5 through Table 8.

TABLE 5 Fifth Embodiment Radius of Refractive Abbe Aspheric Coefficients Curvature(r_(i)) Interval(d_(i)) Index(N_(i)) Number(ν_(i)) K A_(o) B_(o) C_(o) D_(o) r₁ = 0.356 1.667 −6.182 −4.554e+1  −1.638e+3 −9.416e+4 d₁ = 0.1827 N₁ = 1.5304 ν1 = 56.0 r₂ = −17.782  2.624e+3 −7.506 1.246e+1 −6.110e+3 −4.034e+4 d₂ = 0.0000 r3 = ∞ d₃ = 0.1167 r₄ = −0.219  7.041e−2 1.077e+1 5.294e+2 −4.468e+3 −1.464e+5 d₄ = 0.1251 N₄ = 1.6070 ν4 = 27.0 r₅ = −0.344 −6.306e−1 4.833e−2 4.434e+2 −3.444e+3  3.611e+3 d₅ = 0.1000 r₆ = 0.631 −3.669e+1 −4.933 5.289e+1 −2.673e+2  4.585e+2 d₆ = 0.2074 N₆ = 1.5304 ν6 = 56.0 r₇ = 0.537 −1.751e+1 −4.574 2.023e+1 −5.507e+1  1.005e+1 d₇ = 0.3889 r₈ = ∞ Focal Length f = 1.00 mm F Number F_(no) = 3.4 Image Height 2Y = 1.28 mm f₁ = 0.66 mm f₂ = −1.58 mm f₃ = −28.53 mm

TABLE 6 Sixth Embodiment Radius of Refractive Abbe Aspheric Coefficients Curvature(r_(i)) Interval(d_(i)) Index(N_(i)) Number(ν_(i)) K A_(o) B_(o) C_(o) D_(o) r₁ = 0.356 1.657 −6.318 −4.259e+1  −1.573e+3 −1.003e+5 d₁ = 0.1827 N₁ = 1.5304 ν₁ = 56.0 r₂ = −17.782  1.039e+4 −7.887 1.308e+1 −5.938e+3 −5.026e+4 d₂ = 0.0000 r₃ = ∞ d₃ = 0.1167 r₄ = −0.217  9.362e−2 1.061e+1 5.293e+2 −4.194e+3 −1.679e+5 d₄ = 0.1260 N₄ = 1.5830 ν₄ = 30.0 r₅ = −0.347 −6.665e−1 2.110e−1 4.439e+2 −3.472e+3  2.977e+3 d₅ = 0.1000 r₆ = 0.622 −3.304e+1 −4.719 5.254e+1 −2.687e+2  4.934e+2 d₆ = 0.2074 N₆ = 1.5304 ν₆ = 56.0 r₇ = 0.537 −1.674e+1 −4.460 1.976e+1 −5.375e+1  1.997e+1 d₇ = 0.3861 r₈ = ∞ Focal Length f = 1.00 mm F Number F_(no) = 3.4 Image Height 2Y = 1.28 mm f₁ = 0.66 mm f₂ = −1.53 mm f₃ = −46.94 mm

TABLE 7 Seventh Embodiment Radius of Refractive Abbe Aspheric Coefficients Curvature(r_(i)) Interval(d_(i)) Index(N_(i)) Number(ν_(i)) K A_(o) B_(o) C_(o) D_(o) r₁ = 0.356  1.299 −5.360 −6.871e+1   1.240e+3 −1.044e+5 d₁ = 0.1826 N₁ = 1.5300 ν1 = 56.0 r₂ = −8.887  4.898e+2 −6.933 7.254e+1 −5.561e+3 −8.331e+3 d₂ = 0.0000 r₃ = ∞ d₃ = 0.1167 r₄ = −0.227 −1.267e−1 1.717e+1 4.396e+2 −7.141e+3 −7.639e+4 d₄ = 0.1244 N₄ = 1.5830 ν4 = 30.0 r₅ = −0.318 −2.311  2.888 4.437e+2 −2.915e+3 −9.266e+3 d₅ = 0.0800 r₆ = 1.092 −1.866e+2 −5.342 6.070e+1 −2.726e+2  4.963e+2 d₆ = 0.2073 N₆ = 1.5300 ν6 = 56.0 r₇ = 0.568 −2.238e+1 −5.370 2.847e+1 −1.228e+2  1.880e+2 d₇ = 0.3810 r₈ = ∞ Focal Length f = 1.00 mm F Number F_(no) = 3.4 Image Height 2Y = 1.28 mm f₁ = 0.65 mm f₂ = −2.71 mm f₃ = −2.59 mm

TABLE 8 Eighth Embodiment Radius of Refractive Abbe Aspheric Coefficients Curvature(r_(i)) Interval(d_(i)) Index(N_(i)) Number(ν_(i)) K A_(o) B_(o) C_(o) D_(o) r₁ = 0.356  1.300 −5.677 −6.000e+1   3.486e+2 −1.118e+5 d₁ = 0.1826 N₁ = 1.5300 ν₁ = 56.0 r₂ = −8.887  2.300e+3 −8.034 3.438e+1 −5.859e+3 −3.092e+4 d₂ = 0.0000 r₃ = ∞ d₃ = 0.1167 r₄ = −0.216 −1.037e−1 1.815e+1 4.097e+2 −5.808e+3 −1.507e+5 d₄ = 0.1244 N₄ = 1.5830 ν₄ = 30.0 r₅ = −0.303 −2.117  3.302 4.494e+2 −3.010e+3 −1.106e+4 d₅ = 0.0511 r₆ = 1.186 −1.850e+2 −5.012 6.129e+1 −2.753e+2  4.580e+2 d₆ = 0.2073 N₆ = 1.5300 ν₆ = 56.0 r₇ = 0.665 −2.815e+1 −5.570 2.695e+1 −1.195e+2  1.852e+2 d₇ = 0.4222 r₈ = ∞ Focal Length f = 1.00 mm F Number F_(no) = 3.4 Image Height 2Y = 1.28 mm f₁ = 0.65 mm f₂ = −2.67 mm f₃ = −3.32 mm

FIFTH EMBODIMENT

Zeonex E48R was used as the material of the first lens L1 and third lens L3, and the fluorene polyester EP-4000 (EP-4000 is a product number of Mitsubishi Gas Chemical Co., Inc.) was used as the material of the second lens L2.

(A) The object-side radius of curvature r₁ of the first lens L1 is r₁=0.356 mm.

(B) The image-side radius of curvature r₂ of the first lens L1 is r₂=−17.782 mm.

(C) The interval D along the optical axis between the second lens L2 and the third lens L3 is D=0.1000 mm.

(D) The optical length L is L=1.1208 mm.

(E) The image height (length of the diagonal line in the rectangular light-receiving area) 2Y is 2Y=2×0.64=1.28 mm.

(F) The focal length f₁ of the first lens L1 is f₁=0.66 mm.

Hence: |r ₁ /r ₂|=0.356/−17.7821=0.020,  (2-1) D/f=0.1000/1.00=0.1000,  (2-2) L/2Y=1.121/1.28=0.8756, and  (2-3) f ₁ /f=0.66/1.00=0.66.  (2-4)

Hence the lens system of the fifth Embodiment satisfies each of the following condition equations (2-1) through (2-4). 0.01<|r ₁ /r ₂|<0.05  (2-1) 0.05<D/f≦0.1  (2-2) 0.6<L/2Y<0.9  (2-3) 0.5<f ₁ /f<0.7  (2-4)

In the following, the condition equations of the second invention are taken to refer to the above four equations (2-1) through (2-4).

As shown in Table 5, the diaphragm S2 is provided at a position between the first lens L1 and the second lens L2. That is, the diaphragm surface is planar, and so in Table 5 r₃=∞, and the diaphragm S2 is positioned at the position of the plane r₃. The F number is 3.4.

FIG. 19 is a cross-sectional view of the pickup lens of the fifth Embodiment. A sufficiently long back focus relative to the 1.00 mm focal length of 0.389 mm is secured.

FIG. 20 shows the distortion aberration curve 120, FIG. 21 shows the astigmatic aberration curves (the aberration curve 122 in the meridional plane and the aberration curve 124 in the sagittal plane), and FIG. 22 shows the chromatic/spherical aberration curves (the aberration curve 126 for the C line, aberration curve 128 for the d line, aberration curve 130 for the e line, aberration curve 132 for the F line, and aberration curve 134 for the g line).

The vertical axes of the aberration curves in FIG. 20 and FIG. 21 indicate the distance from the optical axis of the image height, as a percentage. In FIG. 20 and FIG. 21, 100% on the vertical axes corresponds to 0.640 mm. The vertical axis for the aberration curve in FIG. 22 indicates the distance of incidence h (F number); the maximum corresponds to 3.4. The horizontal axis in FIG. 22 indicates the aberration magnitude.

The absolute value of distortion aberration is maximum, at 0.3310%, at an image height of 60% (image height 0.384 mm). At image heights of 0.640 mm or less, the absolute value of the aberration is within 0.3310%.

The absolute value of astigmatic aberration is maximum in the meridional plane, at 0.0196 mm, at an image height of 100% (image height 0.640 mm). At image heights of 0.640 mm or less, the absolute value of the aberration is within 0.0196 mm.

The absolute value of chromatic/spherical aberration is maximum, at 0.0114 mm, for the g line of the aberration curve 134 at a distance of incidence h of 30%, and the absolute value of the aberration is within 0.0114 mm.

SIXTH EMBODIMENT

ZEONEX E48R was used as the material of the first lens L1 and third lens L3, and polycarbonate was used as the material of the second lens L2.

(A) The object-side radius of curvature r₁ of the first lens L1 is r₁=0.356 mm.

(B) The image-side radius of curvature r₂ of the first lens L1 is r₂=−17.782 mm.

(C) The interval D along the optical axis between the second lens L2 and the third lens L3 is D=0.1000 mm.

(D) The optical length L is L=1.119 mm.

(E) The image height (length of the diagonal line in the rectangular light-receiving area) 2Y is 2Y=2×0.64=1.28 mm.

(F) The focal length f₁ of the first lens L1 is f₁=0.66 mm.

Hence: |r ₁ /r ₂|=|0.356/−17.782|=0.020,  (2-1) D/f=0.100/1.00=0.100,  (2-2) L/2Y=1.119/1.28=0.874, and  (2-3) f ₁ /f=0.66/1.00=0.66.  (2-4)

Hence the lens system of the sixth Embodiment satisfies each of the following condition equations (2-1) through (2-4). 0.01<|r ₁ /r ₂|<0.05  (2-1) 0.05<D/f≦0.1  (2-2) 0.6<L/2Y<0.9  (2-3) 0.5<f ₁ /f<0.7  (2-4)

In the following, the condition equations of the second invention are taken to refer to the above four equations (2-1) through (2-4).

As shown in Table 6, the diaphragm S2 is provided at a position between the first lens L1 and the second lens L2. That is, the diaphragm surface is planar, and so in Table 6 r₃=∞, and the diaphragm S2 is positioned at the position of the plane r₃. The F number is 3.4.

FIG. 23 is a cross-sectional view of the pickup lens of the sixth Embodiment. A sufficiently long back focus relative to the 1.00 mm focal length of 0.386 mm is secured.

FIG. 24 shows the distortion aberration curve 136, FIG. 25 shows the astigmatic aberration curves (the aberration curve 138 in the meridional plane and the aberration curve 140 in the sagittal plane), and FIG. 26 shows the chromatic/spherical aberration curves (the aberration curve 142 for the C line, aberration curve 144 for the d line, aberration curve 146 for the e-line, aberration curve 148 for the F line, and aberration curve 150 for the g line).

The vertical axes of the aberration curves in FIG. 24 and FIG. 25 indicate the distance from the optical axis of the image height, as a percentage. In FIG. 24 and FIG. 25, 100% on the vertical axes corresponds to 0.640 mm. The vertical axis for the aberration curve in FIG. 26 indicates the distance of incidence h (F number); the maximum corresponds to 3.4. The horizontal axis in FIG. 26 indicates the aberration magnitude.

The absolute value of distortion aberration is maximum, at 0.2936%, at an image height of 60% (image height 0.384 mm). At image heights of 0.640 mm or less, the absolute value of the aberration is within 0.2963%.

The absolute value of astigmatic aberration is maximum in the sagittal plane, at 0.0221 mm, at an image height of 100% (image height 0.640 mm). At image heights of 0.640 mm or less, the absolute value of the aberration is within 0.0221 mm.

The absolute value of chromatic/spherical aberration is maximum, at 0.0129 mm, for the g line of the aberration curve 150 at a distance of incidence h of 30%, and the absolute value of the aberration is within 0.0129 mm.

SEVENTH EMBODIMENT

ZEONEX E48R was used as the material of the first lens L1 and third lens L3, and polycarbonate was used as the material of the second lens L2.

(A) The object-side radius of curvature r₁ of the first lens L1 is r₁=0.356 mm.

(B) The image-side radius of curvature r₂ of the first lens L1 is r₂=−8.887 mm.

(C) The interval D along the optical axis between the second lens L2 and the third lens L3 is D=0.080 mm.

(D) The optical length L is L=1.092 mm.

(E) The image height (length of the diagonal line in the rectangular light-receiving area) 2Y is 2Y=2×0.64=1.28 mm.

(F) The focal length f₁ of the first lens L1 is f₁=0.65 mm.

Hence: |r ₁ /r ₂|=|0.356/−8.887|=0.04,  (2-1) D/f=0.080/1.00=0.08,  (2-2) L/2Y=1.092/1.28=0.8531, and  (2-3) f ₁ /f=0.65/1.00=0.65.  (2-4)

Hence the lens system of the seventh Embodiment satisfies each of the following condition equations (2-1) through (2-4). 0.01<|r ₁ /r ₂|<0.05  (2-1) 0.05<D/f≦0.1  (2-2) 0.6<L/2Y<0.9  (2-3) 0.5<f ₁ /f<0.7  (2-4)

In the following, the condition equations of the second invention are taken to refer to the above four equations (2-1) through (2-4).

As shown in Table 7, the diaphragm S2 is provided at a position between the first lens L1 and the second lens L2. That is, the diaphragm surface is planar, and so in Table 7 r₃=∞, and the diaphragm S2 is positioned at the position of the plane r₃. The F number is 3.4.

FIG. 27 is a cross-sectional view of the pickup lens of the seventh Embodiment. A sufficiently long back focus relative to the 1.00 mm focal length of 0.381 mm is secured.

FIG. 28 shows the distortion aberration curve 152, FIG. 29 shows the astigmatic aberration curves (the aberration curve 154 in the meridional plane and the aberration curve 156 in the sagittal plane), and FIG. 30 shows the chromatic/spherical aberration curves (the aberration curve 158 for the C line, aberration curve 160 for the d line, aberration curve 162 for the e line, aberration curve 164 for the F line, and aberration curve 166 for the g line).

The vertical axes of the aberration curves in FIG. 28 and FIG. 29 indicate the distance from the optical axis of the image height, as a percentage. In FIG. 28 and FIG. 29, 100% on the vertical axes corresponds to 0.640 mm. The vertical axis for the aberration curve in FIG. 30 indicates the distance of incidence h (F number); the maximum corresponds to 3.4. The horizontal axis in FIG. 30 indicates the aberration magnitude.

The absolute value of distortion aberration is maximum, at 0.3963%, at an image height of 80% (image height 0.512 mm). At image heights of 0.640 mm or less, the absolute value of the aberration is within 0.3963%.

The absolute value of astigmatic aberration is maximum in the meridional plane, at 0.0579 mm, at an image height of 100% (image height 0.640 mm). At image heights of 0.640 mm or less, the absolute value of the aberration is within 0.0579 mm.

The absolute value of chromatic/spherical aberration is maximum, at 0.0154 mm, for the g line of the aberration curve 166 at a distance of incidence h of 30%, and the absolute value of the aberration is within 0.0154 mm.

EIGHTH EMBODIMENT

ZEONEX E48R was used as the material of the first lens L1 and third lens L3, and polycarbonate was used as the material of the second lens L2.

(A) The object-side radius of curvature r₁ of the first lens L1 is r₁=0.356 mm.

(B) The image-side radius of curvature r₂ of the first lens L1 is r₂=−8.887 mm.

(C) The interval D along the optical axis between the second lens L2 and the third lens L3 is D=0.0511 mm.

(D) The optical length L is L=1.104 mm.

(E) The image height (length of the diagonal line in the rectangular light-receiving area) 2Y is 2Y=2×0.64=1.28 mm.

(F) The focal length f₁ of the first lens L1 is f₁=0.65 mm.

Hence: |r ₁ /r ₂|=|0.356/−8.887|=0.04,  (2-1) D/f=0.0511/1.00=0.0511,  (2-2) L/2Y=1.104/1.28=0.8627, and  (2-3) f ₁ /f=0.65/1.00=0.65.  (2-4)

Hence the lens system of the eighth Embodiment satisfies each of the following condition equations (2-1) through (2-4). 0.01<|r ₁ /r ₂|<0.05  (2-1) 0.05<D/f≦0.1  (2-2) 0.6<L/2Y<0.9  (2-3) 0.5<f ₁ /f<0.7  (2-4)

In the following, the condition equations of the second invention are taken to refer to the above four equations (2-1) through (2-4).

As shown in Table 8, the diaphragm S2 is provided at a position between the first lens L1 and the second lens L2. That is, the diaphragm surface is planar, and so in Table 8 r₃=∞, and the diaphragm S2 is positioned at the position of the plane r₃. The F number is 3.4.

FIG. 31 is a cross-sectional view of the pickup lens of the eighth Embodiment. A sufficiently long back focus relative to the 1.00 mm focal length of 0.422 mm is secured.

FIG. 32 shows the distortion aberration curve 168, FIG. 33 shows the astigmatic aberration curves (the aberration curve 170 in the meridional plane and the aberration curve 172 in the sagittal plane), and FIG. 34 shows the chromatic/spherical aberration curves (the aberration curve 174 for the C line, aberration curve 176 for the d line, aberration curve 178 for the e line, aberration curve 180 for the F line, and aberration curve 182 for the g line).

The vertical axes of the aberration curves in FIG. 32 and FIG. 33 indicate the distance from the optical axis of the image height, as a percentage. In FIG. 32 and FIG. 33, 100% on the vertical axes corresponds to 0.640 mm. The vertical axis for the aberration curve in FIG. 34 indicates the distance of incidence h (F number); the maximum corresponds to 3.4. The horizontal axis in FIG. 34 indicates the aberration magnitude.

The absolute value of distortion aberration is maximum, at 0.3489%, at an image height of 100% (image height 0.640 mm). At image heights of 0.640 mm or less, the absolute value of the aberration is within 0.3489%.

The absolute value of astigmatic aberration is maximum in the meridional plane, at 0.0344 mm, at an image height of 100% (image height 0.640 mm). At image heights of 0.640 mm or less, the absolute value of the aberration is within 0.0344 mm.

The absolute value of chromatic/spherical aberration is maximum, at 0.0154 mm, for the g line of the aberration curve 182 at a distance of incidence h of 30%, and the absolute value of the aberration is within 0.0154 mm.

As is clear from the explanations of the pickup lenses of the first and second inventions, by designing pickup lenses with the respective lens configurations so as to satisfy the condition equations (1-1) through (1-4) or (2-1) through (2-4), the problems to be resolved by this invention can be resolved. That is, a pickup lens is obtained in which the various aberrations are satisfactorily corrected, a sufficient back focus is obtained, and moreover a short optical length is secured.

In the above-described embodiments, cycloolefin plastics were used in the first lens L1 and third lens L3, and polycarbonate or fluorene polyester plastics were used in the second lens L2; but plastic materials other than those described in the embodiments, as well as materials other than plastics, such as for example molded glass, can of course also be used, so long as the various conditions described in the embodiments are satisfied.

INDUSTRIAL APPLICABILITY

As explained above, by means of pickup lenses of the first and second inventions, various aberrations are satisfactorily corrected, satisfactory images are obtained despite the short optical length, and a sufficient back focus can be secured.

Based on the above explanations, the pickup lenses of this invention can be utilized not only as the camera lenses incorporated in portable telephone sets, personal computers, and digital cameras, but also as camera lenses incorporated in portable information terminals (PDAs or Personal Digital Assistants), as camera lenses incorporated in toys comprising image recognition functions, and as camera lenses incorporated in equipment for monitoring, inspection, or crime prevention. 

1. A pickup lens, comprising: an aperture diaphragm S1, a first lens L1, a second lens L2, and a third lens L3, and being configured by arranging in order, from an object side to an image side, said aperture diaphragm S1, said first lens L1, said second lens L2, and said third lens L3, and wherein said first lens L1 is a lens having positive refractive power, with convex surfaces directed toward the object side and toward the image side; said second lens L2 is a lens having negative refractive power, in a meniscus shape with the convex surface directed toward the image side; said third lens L3 is a lens having negative refractive power, in a meniscus shape with a convex surface directed toward the object side; both surfaces of said first lens L1 are aspherical, both surfaces of said second lens L2 are aspherical, and both surfaces of said third lens L3 are aspherical; and the following conditions are satisfied: 0.01<|r ₂ /r ₃|<0.05  (1-1) 0.05<D/f≦0.1  (1-2) 0.6<L/2Y<0.9  (1-3) 0.5<f ₁ /f<0.7  (1-4) where, f: combined focal length of said pickup lens r₂: radius of curvature of the object-side surface of said first lens L1 in the vicinity of the optical axis r₃: radius of curvature of the image-side surface of said first lens L1 in the vicinity of the optical axis D: interval between said second lens L2 and said third lens L3 along the optical axis L: distance in air along the optical axis from the object-side surface of said first lens L1 to the image plane (optical length) 2Y: length of a diagonal line in an effective picture area of a solid-state image pickup element installed at an image plane of said pickup lens f₁: focal length of said first lens L1.
 2. The pickup lens according to claim 1, wherein said second lens L2 has a material with a higher refractive index than refractive indices of materials of said first lens L1 and said third lens L3, and the said second lens L2 has a material with a smaller Abbe number than Abbe numbers of materials of said first lens L1 and said third lens L3.
 3. The pickup lens according to claim 1, wherein said first lens L1 and said third lens L3 are formed using a cycloolefin plastic as a material, and said second lens L2 is formed using a fluorene polyester as a material.
 4. The pickup lens according to claim 1, wherein said first lens L1 and said third lens L3 are formed using a cycloolefin plastic as a material, and said second lens L2 is formed using a polycarbonate as a material.
 5. A pickup lens, comprising: a first lens L1, an aperture diaphragm S2, a second lens L2, and a third lens, L3, and being configured by arranging in order, from an object side to an image side, said first lens L1, said aperture diaphragm S2, said second lens L2, and said third lens L3, and wherein said first lens L1 is a lens having positive refractive power, with convex surfaces directed toward the object side and toward the image side; said second lens L2 is a lens having negative refractive power, in a meniscus shape with the convex surface directed toward the image side; said third lens L3 is a lens having negative refractive power, in a meniscus shape with a convex surface directed toward the object side; both surfaces of said first lens L1 are aspherical, both surfaces of said second lens L2 are aspherical, and both surfaces of said third lens L3 are aspherical; and the following conditions are satisfied: 0.01<|r ₁ /r ₂|<0.05  (2-1) 0.05<D/f≦0.1  (2-2) 0.6<L/2Y<0.9  (2-3) 0.5<f ₁ /f<0.7  (2-4) where, f: combined focal length of said pickup lens r₁: radius of curvature of the object-side surface of said first lens L1 in the vicinity of the optical axis r₂: radius of curvature of the image-side surface of said first lens L1 in the vicinity of the optical axis D: interval between said second lens L2 and said third lens L3 along the optical axis L: distance in air along the optical axis from the object-side surface of said first lens L1 to the image plane (optical length) 2Y: length of a diagonal line in an effective picture area of a solid-state image pickup element installed at an image plane of said pickup lens f₁: focal length of said first lens L1.
 6. The pickup lens according to claim 5, wherein said second lens L2 has a material with a higher refractive index than refractive indices of materials of said first lens L1 and said third lens L3, and the said second lens L2 has a material with a smaller Abbe number than Abbe numbers of materials of said first lens L1 and said third lens L3.
 7. The pickup lens according to claim 5, wherein said first lens L1 and said third lens L3 are formed using a cycloolefin plastic as a material, and said second lens L2 is formed using a fluorene polyester as a material.
 8. The pickup lens according to claim 5, wherein said first lens L1 and said third lens L3 are formed using a cycloolefin plastic as a material, and said second lens L2 is formed using a polycarbonate as a material. 